Abstract
This model explains why breakup has been observed as low as L = 5‐6 and predicts that a higher concentration of O+ in the plasma sheet will permit breakup at such low L values. The establishment of a coupled current structure within a single arc leads to a quasi‐stable system i.e. the pre‐breakup regime. Perturbation of the pre‐breakup structure leads to an instability criterion. Certain quiescent configurations are inherently unstable. Transitions from a stable to an unstable situation can trigger a rapid poleward expansion of the quiescent arc or substorm breakup. The kinetic energy of injected plasma from the magnetotail supplies the energy for breakup.
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